US3753163A - Electromagnetic wave-elastic wave transducer and method - Google Patents
Electromagnetic wave-elastic wave transducer and method Download PDFInfo
- Publication number
- US3753163A US3753163A US00211976A US3753163DA US3753163A US 3753163 A US3753163 A US 3753163A US 00211976 A US00211976 A US 00211976A US 3753163D A US3753163D A US 3753163DA US 3753163 A US3753163 A US 3753163A
- Authority
- US
- United States
- Prior art keywords
- wave
- medium
- elastic
- magnetic field
- electromagnetic
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000000034 method Methods 0.000 title claims description 17
- 238000006243 chemical reaction Methods 0.000 claims abstract description 29
- 230000005418 spin wave Effects 0.000 claims abstract description 28
- 230000005641 tunneling Effects 0.000 claims abstract description 10
- 230000000644 propagated effect Effects 0.000 claims abstract description 6
- 230000005291 magnetic effect Effects 0.000 claims description 34
- 230000003247 decreasing effect Effects 0.000 claims description 12
- 230000000694 effects Effects 0.000 claims description 11
- 230000005415 magnetization Effects 0.000 claims description 10
- 230000002463 transducing effect Effects 0.000 claims description 8
- 230000000630 rising effect Effects 0.000 claims description 5
- 230000007423 decrease Effects 0.000 claims description 3
- 230000001629 suppression Effects 0.000 claims description 3
- 239000000463 material Substances 0.000 claims description 2
- 230000001902 propagating effect Effects 0.000 claims description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 6
- 239000013078 crystal Substances 0.000 description 5
- 239000004020 conductor Substances 0.000 description 3
- 229910052742 iron Inorganic materials 0.000 description 3
- 229910000859 α-Fe Inorganic materials 0.000 description 3
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 2
- 238000010276 construction Methods 0.000 description 2
- 229910052733 gallium Inorganic materials 0.000 description 2
- 239000002223 garnet Substances 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 230000026683 transduction Effects 0.000 description 2
- 238000010361 transduction Methods 0.000 description 2
- OBOSXEWFRARQPU-UHFFFAOYSA-N 2-n,2-n-dimethylpyridine-2,5-diamine Chemical compound CN(C)C1=CC=C(N)C=N1 OBOSXEWFRARQPU-UHFFFAOYSA-N 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000005229 chemical vapour deposition Methods 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000002050 diffraction method Methods 0.000 description 1
- 238000007598 dipping method Methods 0.000 description 1
- 229910052738 indium Inorganic materials 0.000 description 1
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical group [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- FBAFATDZDUQKNH-UHFFFAOYSA-M iron chloride Chemical compound [Cl-].[Fe] FBAFATDZDUQKNH-UHFFFAOYSA-M 0.000 description 1
- MTRJKZUDDJZTLA-UHFFFAOYSA-N iron yttrium Chemical compound [Fe].[Y] MTRJKZUDDJZTLA-UHFFFAOYSA-N 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 239000000523 sample Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
- 239000013589 supplement Substances 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/02—Details
- H03H9/125—Driving means, e.g. electrodes, coils
Definitions
- the present invention relates to electromagnetic wave-elastic wave transducers and methods, being particularly directed to such devices involving magnetoelastic media, such as YIG crystals and the like.
- An object of the invention is to provide a new and improved method of transducing and an improved transducer structure, particularly adapted for YIG and similar magneto-elastic structures, that enables use with extremely high X-band microwave frequencies and increased powers.
- a further object is to provide a novel transducer of more general utility, as well.
- the invention in one of its aspects, involves the provision of tunneling spin-wave conversion (electromagnetic-to-spin wave energy) and spin wave-toelastic wave conversion in successive transduction layers near an end of a magneto-elastic medium. Preferred constructional details are hereinafter discussed.
- FIGURE is a greatly magnified side elevation of a preferred construction embodying the invention, with operational wave forms illustrated thereupon to describe the performance.
- a YIG or similar magnetoelastic medium including Ga-doped YIG, Mn-doped YIG, Mn-Ga-doped YIG, Eu-doped YIG, Li-ferrite, as illustrations, is shown at 2, provided at its opposite ends with similar terminal transducing structures 1 and 1', respectively connected with electromagnetic-wave energy conductors, illustrated and described herein generically as antenna or probe structures 3 and 3 for the input and output transmission of electromagnetic currents.
- a steeply decreasing magnetic field profile A is set up through the transducer layer 1, leveling off through the medium 2 at B, and steeply rising at the other transducer end 1', as shown at C.
- the transducing regions I, and I and the regions A and C will, as later explained, preferably be very thin terminal layers of the relatively long medium 2, enabling high frequency and high power operation.
- the antennas at 3 and 3' may be thin wires or thin deposited strips or conductors.
- a novel transducing operation can be achieved by appropriate orientation and value of a bias magnetic field H applied axially along the medium 2, in this example, to intersect the steeply decreasing and steeply rising magnetic field profile end characteristics A and C at intermediate points P and P, respectively.
- the region R represents the layer where the region l of the steeply decreasing or falling profile portion .A applies; and successive adjacent regions R and R correspond to regions [I and III of the field profile portion A.
- the value of H is selected so as to achieve cut off of the electromagnetic wave input at 3 over the region R,, and suppression of any possible conversion of the electromagnetic energy to spin waves therein.
- the wavelength of the spin waves (SW) will decrease with decreasing amplitude as they are propagated through the region R as shown, under the decreasing field characteristic II of the magnetic field profile portion A, until the point P" of the medium is reached at which the wavelength is sufficiently decreased to effect splitting conversion from spin waves (SW) to elastic waves (ELW), which are then propagated through the next adjacent region R (where the magnetization profile portion Ill applies), and thence into and through the medium 2.
- the successive regions R R and R should have successively increasing saturation magnetization. This may be effected, for example, by growing epitaxial YIG layers at this end of the YIG medium 2 (and at the other end 1 introducing successively increasing amounts of, for example, gallium doping to replace progressively more iron in the YIG. Such doping, while not previously effected for these purposes, may be accomplished, for example, by techniques such as described in Magnetic Effects of Indium and Gallium Substitutions in Yttrium Iron Garnet", Anderson et al., Journal of the Physical Society of Japan, Vol.
- the epitaxial growth technique for forming the layers may be carried out in serveral ways including chemical vapor deposition and molten dipping.
- yttrium chloride, iron chloride andthe like have been mixed within a quartz tube furnace and vapor-deposited at high temperature on a Gd-Ga garnet substrate to produce the desired depositions.
- the chemical constituents are prepared in molten form and the substrate is suecessively dipped therein to build up the layers.
- a method of transducing electromagnetic waves into elastic waves and vice versa that comprises, producing a magnetic field profile along a magneto-elasticwave supporting medium that steeply decreases at one end and increases at the other end; contacting electromagnetic wave antennae to the said ends of the medium; applying a bias magnetic field to the medium and adjusting the value and orientation thereof to cause its magnetic field operating-level line to intersect the steeply decreasing and increasing portions of the magnetic field profile at intermediate points of such portions such that, as the electromagnetic wave launches into the medium at said one end, it initially encounters in a first region preceding the said intermediate point, both electromagnetic-wave-cutoff and spin wave-conversion-suppression, forcing tunneling through said first region to the next adjacent region at which conversion to spin waves of successively decreasing wavelength occurs, which, in turn, are propagated to a further adjacent region of said steeply decreasing profile portion at which the wavelength has become sufficiently small to effect conversion from spin-wave to elastic-wave energy; and propagating the elastic wave energy into the medium; with the reverse conversion operation occuring at the said other end
- a method of transducing between electromagnetic waves and elastic waves that comprises, producing a steeply changing magnetic field profile at an end of a magneto-elastic-wave supporting medium; contacting an electro-magnetic wave antenna to said end of the medium; applying a bias magnetic field to the medium of such direction and valve that its magnetic field operating-level line intersects the steeply changing profile at an intermediate point thereof defining a first region thereof, where electromagnetic wave energy is cutoff and spin-wave conversion thereof is suppressed to force tunneling through said first region, with conversion to spin waves of successively changing wavelength occuring along the next adjacent region of the steeply changing profile up to the point where such wavelength is sufficiently small to effect conversion between spin wave and elastic wave energy; the elastic wave energy being supported in the medium adjacent the said end.
- An electromagnetic wave-elastic wave transducer having, in combination, a magneto-elastic-wave supporting medium provided at one end with an electromagnetic wave antenna, means for establishing at said one end a magnetic field profile that steeply changes over a narrow portion of the medium near said one end, means for applying a bias magnetic field to the medium of such direction and value that its magnetic field operating-level line intersects the steeply changing profile at an intermediate point defining a first region thereof followed by second and third adjacent regions of the steeply changing profile, the field being adjusted to produce spin electromagnetic-wave cutoff and spin wave conversion suppression along the said first region to force tunneling therealong, with conversion to spin waves of successively changing wavelength along the said second region and with the third region disposed where such wavelength is sufficiently small to effect conversion between spin wave and elastic wave energy; the medium adjacent said one end supporting the elastic wave energy therein.
- An electromagnetic wave-elastic wave transducer as claimed in claim 4 and in which the means provided to produce said steeply changing magnetic profile comprises a further medium disposed adjacent the firstnamed medium but of different saturation magnetizat a t a a
Landscapes
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US21197671A | 1971-12-27 | 1971-12-27 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US3753163A true US3753163A (en) | 1973-08-14 |
Family
ID=22789027
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US00211976A Expired - Lifetime US3753163A (en) | 1971-12-27 | 1971-12-27 | Electromagnetic wave-elastic wave transducer and method |
Country Status (6)
| Country | Link |
|---|---|
| US (1) | US3753163A (OSRAM) |
| JP (1) | JPS4877785A (OSRAM) |
| FR (1) | FR2166104A1 (OSRAM) |
| GB (1) | GB1382160A (OSRAM) |
| IT (1) | IT972967B (OSRAM) |
| NL (1) | NL7217679A (OSRAM) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3918012A (en) * | 1973-08-03 | 1975-11-04 | Commissariat Energie Atomique | Method and device for providing a variable delay line |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5136175B2 (ja) * | 2008-04-11 | 2013-02-06 | 日本電気株式会社 | 周波数変換器および周波数変換方法 |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3249882A (en) * | 1962-12-17 | 1966-05-03 | Gen Electric | Spin and phonon spin traveling wave parametric amplifiers and spin wave delay lines |
| US3309628A (en) * | 1965-05-07 | 1967-03-14 | Teledyne Inc | Yig broadband variable acoustic delay line |
| US3353118A (en) * | 1964-05-19 | 1967-11-14 | Teledyne Inc | Magnetostatic wave variable delay apparatus |
| US3444484A (en) * | 1967-04-03 | 1969-05-13 | Raytheon Co | Solid state delay line for propagation of microwave frequency energy in spin wave mode |
| US3530302A (en) * | 1967-06-14 | 1970-09-22 | Massachusetts Inst Technology | Method of and apparatus for changing frequency power and/or delay time of wave energy |
| US3668568A (en) * | 1969-10-06 | 1972-06-06 | Chu Associates | Signal processing apparatus |
-
1971
- 1971-12-27 US US00211976A patent/US3753163A/en not_active Expired - Lifetime
-
1972
- 1972-12-27 NL NL7217679A patent/NL7217679A/xx unknown
- 1972-12-27 IT IT33643/72A patent/IT972967B/it active
- 1972-12-27 JP JP48004218A patent/JPS4877785A/ja active Pending
- 1972-12-27 FR FR7246507A patent/FR2166104A1/fr not_active Withdrawn
- 1972-12-27 GB GB5961572A patent/GB1382160A/en not_active Expired
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3249882A (en) * | 1962-12-17 | 1966-05-03 | Gen Electric | Spin and phonon spin traveling wave parametric amplifiers and spin wave delay lines |
| US3353118A (en) * | 1964-05-19 | 1967-11-14 | Teledyne Inc | Magnetostatic wave variable delay apparatus |
| US3309628A (en) * | 1965-05-07 | 1967-03-14 | Teledyne Inc | Yig broadband variable acoustic delay line |
| US3444484A (en) * | 1967-04-03 | 1969-05-13 | Raytheon Co | Solid state delay line for propagation of microwave frequency energy in spin wave mode |
| US3530302A (en) * | 1967-06-14 | 1970-09-22 | Massachusetts Inst Technology | Method of and apparatus for changing frequency power and/or delay time of wave energy |
| US3668568A (en) * | 1969-10-06 | 1972-06-06 | Chu Associates | Signal processing apparatus |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3918012A (en) * | 1973-08-03 | 1975-11-04 | Commissariat Energie Atomique | Method and device for providing a variable delay line |
Also Published As
| Publication number | Publication date |
|---|---|
| GB1382160A (en) | 1975-01-29 |
| NL7217679A (OSRAM) | 1973-06-29 |
| FR2166104A1 (OSRAM) | 1973-08-10 |
| IT972967B (it) | 1974-05-31 |
| JPS4877785A (OSRAM) | 1973-10-19 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Hickernell | DC triode sputtered zinc oxide surface elastic wave transducers | |
| US3753163A (en) | Electromagnetic wave-elastic wave transducer and method | |
| DE4121550A1 (de) | Magnetoelastische wellenvorrichtung | |
| US3309628A (en) | Yig broadband variable acoustic delay line | |
| US3244993A (en) | Electronically adjustable spin-wave delay line and parametric amplifier | |
| US3353118A (en) | Magnetostatic wave variable delay apparatus | |
| JPH07105642B2 (ja) | 超電導可変位相シフタ | |
| US4188594A (en) | Fixed frequency filters using epitaxial ferrite films | |
| US3975698A (en) | Fiber acoustic waveguide and system | |
| US3444484A (en) | Solid state delay line for propagation of microwave frequency energy in spin wave mode | |
| US20220385267A1 (en) | Surface acoustic wave device with high electromechanical coupling coefficient based on double-layer electrodes and preparation method thereof | |
| US3218503A (en) | Electron beam devices | |
| Adam | A broadband microwave signal to noise enhancer | |
| US3668568A (en) | Signal processing apparatus | |
| US3249882A (en) | Spin and phonon spin traveling wave parametric amplifiers and spin wave delay lines | |
| Okubo et al. | A new magnetostatic wave delay line using YIG film | |
| AU2003246021A1 (en) | Radio frequency and microwave signals | |
| US3707689A (en) | Electrical signal processing method and apparatus | |
| US4138651A (en) | Multiple magnetic layer composite for magnetostatic surface wave propagation | |
| Hobrecht | Resonant loss for helix traveling wave tubes | |
| Collins | A short history of microwave acoustics | |
| GB773834A (en) | Improvements in or relating to electron wavetubes | |
| US3292114A (en) | Ultrasonic delay line for microwave and higher frequencies | |
| US3753165A (en) | Tunable variable bandwidth magneto-elastic filter and method | |
| US2507358A (en) | Delay transmission line |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| AS | Assignment |
Owner name: LIQUID CRYSTAL TECHNOLOGY, INC., Free format text: SECURITY INTEREST;ASSIGNOR:DAVIS, FREDERICK;REEL/FRAME:003904/0399 Effective date: 19810723 Owner name: BAYBANK MIDDLESEX, SEVEN NEW ENGLAND EXECUTIVE PAR Free format text: LICENSE;ASSIGNOR:CHU ASSOCIATES, INC. A CORP. OF MA;REEL/FRAME:003917/0324 Effective date: 19810724 |